Search results for "ISOSCALAR"

showing 10 items of 91 documents

Measurement of high energy resolution inelastic proton scattering at and close to zero degrees

2009

13 pages, 15 figures.-- Printed version published Jul 1, 2009.

Nuclear and High Energy PhysicsHigh energy resolutionM1 excitationForward scatterCyclotronMeasurement at 0 degreesTRANSITIONSInelastic scatteringDispersion matchingISOVECTORlaw.inventionSHELL NUCLEINuclear physicsNUCLEON-NUCLEON INTERACTIONlawBEAM LINEE1 Coulomb excitationFOCAL-PLANE POLARIMETERInstrumentationInelastic proton scatteringPolarization transfer coefficientsISOSCALARElastic scatteringPhysicsBackground subtractionPolarization transfer coefficientScatteringResolution (electron density)SPIN EXCITATIONSBeamlinePhysics::Accelerator PhysicsMeasurement at 0ºAtomic physicsSPECTROMETER GRAND RAIDENINTERMEDIATE ENERGIES
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Pinning down the strength function for ordinary muon capture on 100Mo

2019

Ordinary muon capture (OMC) on 100Mo is studied both experimentally and theoretically in order to access the weak responses in wide energy and momentum regions. The OMC populates states in 100Nb up to some 50 MeV in excitation energy. For the first time the associated OMC strength function has been computed and compared with the obtained data. The present computations are performed using the Morita-Fujii formalism of OMC by extending the original formalism beyond the leading order. The participant nuclear wave functions are obtained in extended no-core single-particle model space using the spherical version of proton-neutron quasiparticle random-phase approximation (pnQRPA) with two-nucleon…

Nuclear and High Energy PhysicsIsoscalarmuon-capture giant resonanceNuclear Theorydouble beta decaynuclear matrix elementshiukkasfysiikka01 natural sciencesRenormalization0103 physical sciencesordinary muon capture010306 general physicsWave functionNuclear Experimentvalues of weak axial couplingsPhysicsIsovector010308 nuclear & particles physicslcsh:QC1-999Muon captureGiant resonanceQuantum electrodynamicsIsospinQuasiparticleydinfysiikkacapture-rate distributionlcsh:Physics
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Transition probabilities in 31P and 31S : A test for isospin symmetry

2021

International audience; Excited states in the mirror nuclei 31P and 31S were populated in the 1p and 1n exit channels of the reaction 20Ne + 12C, at a beam energy of 33 MeV. The 20Ne beam was delivered for the first time by the Piave-Alpi accelerator of the Laboratori Nazionali di Legnaro. Angular correlations of coincident γ-rays and Doppler-shift attenuation lifetime measurements were performed using the multi-detector array GASP in conjunction with the EUCLIDES charged particle detector. In the observed B(E1) strengths, the isoscalar component, amounting to 24% of the isovector one, provides strong evidence for breaking of the isospin symmetry in the A=31 mass region. Self-consistent bey…

Nuclear and High Energy PhysicsLifetime measurementIsoscalarQC1-999Lifetime measurementslifetime measurements[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesResonance (particle physics)Isospin symmetrytransition probabilitiesNuclear physicsMicroscopic multiphonon modelMirror nucleimirror nuclei0103 physical sciencesMirror nucleiIsospin symmetry; Lifetime measurements; Microscopic multiphonon model; Mirror nuclei; Transition probabilities010306 general physicsmirrorTransition probabilitiesPhysicsIsovector010308 nuclear & particles physicsPhysics31SCharge (physics)31PSymmetry (physics)Charged particleisospin symmetryIsospinmicroscopic multiphonon modelnucleiydinfysiikka
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Isospin mixing and the continuum coupling in weakly bound nuclei

2009

The isospin breaking effects due to the Coulomb interaction in weakly-bound nuclei are studied using the Gamow Shell Model, a complex-energy configuration interaction approach which simultaneously takes into account many-body correlations between valence nucleons and continuum effects. We investigate the near-threshold behavior of one-nucleon spectroscopic factors and the structure of wave functions along an isomultiplet. Illustrative calculations are carried out for the T=1 isobaric triplet. By using a shell-model Hamiltonian consisting of an isoscalar nuclear interaction and the Coulomb term, we demonstrate that for weakly bound or unbound systems the structure of isobaric analog states v…

Nuclear and High Energy PhysicsNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]IsoscalarNuclear TheoryFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)symbols.namesakeQuantum mechanics0103 physical sciencesCoulombSymmetry breakingMirror nucleiNuclear Experiment010306 general physicsWave functionPhysics010308 nuclear & particles physics3. Good healthIsospinsymbols21.10.Sf 21.60.Cs 24.10.Cn 21.10.JxAtomic physicsHamiltonian (quantum mechanics)Nucleon
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Peripheral transverse densities of the baryon octet from chiral effective field theory and dispersion analysis

2017

The baryon electromagnetic form factors are expressed in terms of two-dimensional densities describing the distribution of charge and magnetization in transverse space at fixed light-front time. We calculate the transverse densities of the spin-1/2 flavor-octet baryons at peripheral distances b = O(M_\pi^{-1}) using methods of relativistic chiral effective field theory (\chi EFT) and dispersion analysis. The densities are represented as dispersive integrals over the imaginary parts of the form factors in the timelike region (spectral functions). The isovector spectral functions on the two-pion cut t > 4 M_\pi^2 are calculated using relativistic \chi EFT including octet and decuplet baryons.…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryIsoscalarHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)PionHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesVector meson010306 general physicsNuclear ExperimentPhysicsIsovector010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)HyperonForm factor (quantum field theory)BaryonHigh Energy Physics - PhenomenologyQuantum electrodynamicsHigh Energy Physics::Experiment
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Nature of the light scalar mesons

2005

Despite the apparent simplicity of meson spectroscopy, light scalar mesons cannot be accommodated in the usual $q\bar q$ structure. We study the description of the scalar mesons below 2 GeV in terms of the mixing of a chiral nonet of tetraquarks with conventional $q\bar q$ states. A strong diquark-antidiquark component is found for several states. The consideration of a glueball as dictated by quenched lattice QCD drives a coherent picture of the isoscalar mesons.

Nuclear and High Energy PhysicsParticle physicsMesonNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]IsoscalarHigh Energy Physics::Latticemeson massquark confinementLattice field theoryNuclear TheoryFOS: Physical sciencessparticles01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesquantum chromodynamics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysics010308 nuclear & particles physicsGlueballHigh Energy Physics::PhenomenologyScalar (physics)lattice field theory12.39.-x 12.38.-tFísicaLattice QCDDiquarkHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentchiral symmetries
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Neutrino-nucleus quasi-elastic and 2p2h interactions up to 10 GeV

2013

We extend to 10 GeV results from a microscopic calculation of charged-current neutrino-nucleus reactions that do not produce a pion in the final state. For the class of events coming from neutrino interactions with two nucleons producing two holes (2p2h), limiting the calculation to three-momentum transfers less than 1.2 GeV produces a two-dimensional distribution in momentum and energy transfer that is roughly constant as a function of energy. The cross section for 2p2h interactions approximately scales with the number of nucleons for isoscalar nuclei, similar to the quasi-elastic cross section. When limited to momentum transfers below 1.2 GeV, the cross section is 26% of the quasi-elastic…

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryIsoscalarFOS: Physical sciences01 natural sciences7. Clean energyScatteringNuclear Theory (nucl-th)Nuclear physicsMomentumCross section (physics)High Energy Physics - Phenomenology (hep-ph)Pion0103 physical sciencesNuclear Experiment010306 general physicsNeutrino oscillationPhysicsMeson-exchange currents010308 nuclear & particles physicsMomentum transferHigh Energy Physics - PhenomenologyFísica nuclearHigh Energy Physics::ExperimentNeutrinoNucleonPhysical Review D
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s-wave pion-nucleus optical potential

2007

We calculate the s-wave part of the pion-nucleus optical potential using a unitarized chiral approach that has been previously used to simultaneously describe pionic hydrogen and deuterium data as well as low energy pi N scattering in the vacuum. This energy dependent model allows for additional isoscalar parts in the potential from multiple rescattering. We consider Pauli blocking and pion polarization in an asymmetric nuclear matter environment. Also, higher order corrections of the pi N amplitude are included. The model can accommodate the repulsion required by phenomenological fits, though the theoretical uncertainties are bigger than previously thought. At the same time, we also find a…

Nuclear and High Energy PhysicsParticle physicsscattering amplitude [pi nucleon]Nuclear Theorymedia_common.quotation_subjectIsoscalarpartial waveNuclear TheoryFOS: Physical sciencesAsymmetryrenormalizationNuclear physicsNuclear Theory (nucl-th)symbols.namesakePionPauli exclusion principlemesic atom [deuterium]unitarityddc:530higher-order [Feynman graph]nuclear reaction [pi nucleus]numerical calculationsNuclear Experimentmedia_commonPhysicschiral [symmetry]UnitarityIsovectorN(1440)FísicaNuclear mattermesic atom [hydrogen]propagator [pi]Scattering amplitudenuclear mattersymbolsoptical [potential]correction [vertex function]
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New states as observed by the Crystal Barrel experiment

1993

Abstract The Crystal Barrel Detector has been in operation since October 1989. Results on the analysis of the annihilation of protonium at rest into three pseudoscalars is presented. The π 0 π 0 π 0 final state confirms the existence of ƒ 2 (1520)→π 0 π 0 . In the ηη system of the π 0 ηη final state an isoscalar J PC = 0 ++ resonance with a mass of 1560 MeV/c 2 and a width of 245 MeV/c 2 is observed. The identification with ƒ 0 (1590) is doubtful since the ηη' decay is not observed with the corresponding strength. Our analysis yields an upper limit for the relative branching ratio BR(ƒ 0 (1560)→ηη') BR(ƒ 0 (1560)→ηη) .

Nuclear physicsCrystalPhysicsNuclear and High Energy PhysicsBarrelAnnihilationProtoniumBranching fractionIsoscalarResonanceState (functional analysis)Atomic physicsNuclear Physics A
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Contributions of internal nucleon structure to the nuclear charge and current operators

1983

The relativistic pair current and contributions of nucleon isobars are evaluated in the constituent-quark model. Isovector charge and isoscalar current contributions change substantially compared to previous calculations. The magnetic form factor of the deuteron and the charge form factors of3He and3H are modifed significantly and the previously predicted large differences in the form factors of3He and3H are considerably reduced.

Nuclear physicsPhysicsDeuteriumIsovectorIsoscalarQuantum electrodynamicsNuclear TheoryMagnetic form factorIsobarCharge (physics)Nuclear ExperimentNucleonEffective nuclear chargeIl Nuovo Cimento A
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